Problem 44
Question
In the twin paradox example, Alice boards a spaceship that flies to a space station 3.25 light-years away and then returns with a speed of \(0.650 c .\) This can be viewed in terms of Alice's reference frame. a) Show that Alice must travel with a speed of \(0.914 c\) to establish a relative speed of \(0.650 c\) with respect to Earth when Alice is returning back to Earth. b) Calculate the time duration for Alice's return flight toward Earth with the aforementioned speed.
Step-by-Step Solution
Verified Answer
Answer: Alice must travel at a speed of 0.914c to have a relative velocity of 0.65c with respect to Earth on her return trip. Her return flight will take approximately 2.14 years.
1Step 1: Finding the relative velocity between Earth and Alice on her return
To find Alice's required speed for having a relative velocity of 0.65c with respect to Earth, we need to use the relativistic velocity addition formula:
\(u' = \frac{u+v}{1 + \frac{uv}{c^2}}\)
Here, \(u'\) is the relative velocity, \(u\) is Earth's velocity, \(v\) is Alice's velocity, and \(c\) is the speed of light.
In this case, Alice's spaceship is moving in the opposite direction when returning (\(-0.650c\)). So, we have:
\(u' = 0.650c, u = -0.650c\), and we need to find \(v\).
2Step 2: Using the relativistic velocity addition formula
Plugging the values from Step 1 into the relativistic velocity addition formula, we get:
\(0.650c = \frac{v - 0.650c}{1 - \frac{v(-0.650c)}{c^2}}\)
Next, we solve this equation for \(v\):
\(0.650 = \frac{v - 0.650}{1 + 0.650v} \Rightarrow\)
\(0.650 + 0.650^2v = v - 0.650 \Rightarrow\)
\(v(1 - 0.650^2) = 1.3 \Rightarrow\)
\(v = \frac{1.3}{1 - 0.650^2} = 0.914\)
So, Alice must travel with a speed of \(0.914c\) to have a relative speed of \(0.650c\) with respect to Earth when returning.
3Step 3: Calculating the time for Alice's return flight using time dilation formula
To calculate the time duration of Alice's return flight, we first need to find the distance she travels in her reference frame. We can calculate this by using the Lorentz length contraction formula:
\(L' = L \sqrt{1 - \frac{v^2}{c^2}}\)
Here, \(L = 3.25\,\text{light-years}\) is the distance in Earth's frame, and \(L'\) is the distance in Alice's frame.
Plugging the values into the length contraction formula, we get:
\(L' = 3.25\, \sqrt{1 - \frac{(0.914c)^2}{c^2}}\)
\(L' = 3.25\, \sqrt{1 - 0.914^2} \approx 1.96\,\text{light-years}\)
Now we can use the time dilation formula to find the time duration of Alice's return flight:
\(\Delta t' = \frac{\Delta t}{\sqrt{1 - \frac{v^2}{c^2}}}\)
Here, \(\Delta t'\) is the time duration in Alice's frame, and \(\Delta t\) is the time duration in Earth's frame. We need to find \(\Delta t'\).
Knowing the distance and velocity in Alice's frame, we can find the time duration as:
\(\Delta t' = \frac{L'}{v} = \frac{1.96\,\text{light-years}}{0.914c}\)
\(\Delta t' \approx 2.14\, \text{years}\)
So, the time duration of Alice's return flight with the required speed is approximately 2.14 years.
Key Concepts
Relativistic Velocity Addition FormulaTime DilationLorentz Length ContractionSpecial Relativity
Relativistic Velocity Addition Formula
When Alice travels at a significant fraction of the speed of light, simply adding her spaceship's speed to Earth's would not provide an accurate measure of her relative speed due to the effects of special relativity. This is where the relativistic velocity addition formula comes into play. It corrects for the distortions that arise at high speeds. The formula is:
\[\begin{equation}u = \frac{u + v}{1 + \frac{uv}{c^2}}\tag{1}\text{where:}\end{equation}\]
\[\begin{equation}u = \frac{u + v}{1 + \frac{uv}{c^2}}\tag{1}\text{where:}\end{equation}\]
- \begin{math}u\text{ is the resultant relative velocity.}\text{}
- \begin{math}u\text{ and }v\text{ are the velocities of the two moving objects in any frame.}
- \begin{math}c\text{ is the speed of light in a vacuum.}\text{}
Time Dilation
An astonishing consequence of traveling at relativistic speeds, as shown in Alice's journey, is time dilation. This effect predicts that time moves slower for an observer in motion, compared to an observer at rest. Albert Einstein's special theory of relativity provides the quantitative tool to calculate this temporal discrepancy with the time dilation formula:
\[\begin{equation} \begin{split} \tau = \frac{t}{\begin{math}\begin{vmatrix}1 - \frac{v^2}{c^2}\text{} \begin{math}\begin{vmatrix}\tau\text{is the time experienced by the moving observer (Alice),}\text{} t\text{is the proper time for the stationary observer (Earth),}\text{} v\text{is the velocity of the moving observer, and} c^2\text{is the square of the speed of light.}\text{} For Alice traveling back to Earth, the time dilation formula allows us to determine that she will experience less time than her twin who stays behind on Earth. This time difference is not due to the mechanical workings of clocks but rather to the fundamental nature of time itself as affected by motion at high speeds.
\[\begin{equation} \begin{split} \tau = \frac{t}{\begin{math}\begin{vmatrix}1 - \frac{v^2}{c^2}\text{}
Lorentz Length Contraction
Along with time and velocity, distance also behaves in non-intuitive ways at relativistic speeds. This is manifest in the phenomenon known as Lorentz length contraction. Objects moving relative to an observer will appear shorter along the direction of motion, proportional to their speed:
\[\begin{equation}L' = L\begin{math}\begin{vmatrix}1 - \frac{v^2}{c^2}\text{}\begin{math}L'\end{math}\text{is the contracted length as observed in the moving reference frame (Alice's spaceship),} \end{math}\text{} L\text{is the proper length as measured in the rest frame (Earth),} \begin{math}\text{} v\text{is the velocity of the moving object, and}\text{} \begin{math} c^2\text{is the square of the speed of light.}\text{} In the twin paradox that Alice undergoes, the distance to the target destination appears shorter in her own reference frame than it would appear to someone stationary relative to the space itself, like her twin on Earth. Lorentz contraction is a central aspect of special relativity that enforces the limit that no information or matter can travel faster than the speed of light.
\[\begin{equation}L' = L\begin{math}\begin{vmatrix}1 - \frac{v^2}{c^2}\text{}
Special Relativity
The unity of the concepts described above—relativistic velocity addition, time dilation, and Lorentz length contraction—are encompassed within Einstein's theory of special relativity. This theory fundamentally changed our understanding of space, time, and motion by describing how these are perceived differently by observers in different inertial frames of reference, especially at speeds comparable to the speed of light. It is a cornerstone that reconciled the laws of motion with the constancy of the speed of light.Special relativity can be summarized by two postulates:
- The laws of physics are invariant (identical) in all inertial frames of reference (those moving at constant velocity with respect to each other).
- The speed of light in vacuum is the same for all observers, regardless of the motion of the light source or observer.
Other exercises in this chapter
Problem 42
A rocket ship approaching Earth at \(0.90 c\) fires a missile toward Earth with a speed of \(0.50 c,\) relative to the rocket ship. As viewed from Earth, how fa
View solution Problem 43
In the twin paradox example, Alice boards a spaceship that flies to a space station 3.25 light-years away and then returns with a speed of \(0.65 c\). a) Calcul
View solution Problem 45
Robert, standing at the rear end of a railroad car of length \(100 . \mathrm{m},\) shoots an arrow toward the front end of the car. He measures the velocity of
View solution Problem 46
Consider motion in one spatial dimension. For any velocity \(v,\) define parameter \(\theta\) via the relation \(v=c \tanh \theta\) where \(c\) is the vacuum sp
View solution